SETTINGS SAVED TO FILE

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Particle Data

The structure and operation of the particle data table is described ";?>here. That page also describes how default data properties can be changed. The current page provides the actual default values.

Main settings

Apart from the data itself, the particle data table only contains a few aspects that are available to change:

ParticleData:modeBreitWigner   (default = 4; minimum = 0; maximum = 4)
Selection of particle masses when the mSel(id) is called to provide a new mass:
0 : mass is fixed at the nominal m_0 value.
1 : particles registered as having a mass width are given a mass in the range m_min < m < m_max, according to a truncated nonrelativistic Breit-Wigner, i.e. linear in m.
2 : as above, except that the width is made mass-dependent: Gamma = Gamma_0 * sqrt( (m^2 - m_thr^2) / (m_0^2 - m_thr^2) ) where m is the current mass, m_0 the nominal one and m_thr is the mass threshold, given by the sum of the nominal masses of the decay products. In order to decouple production and decay the threshold is defined as the branching-ratio-weighted average over all allowed decay channels.
3 : particles registered as having a mass width are given a mass in the range m_min < m < m_max, according to a truncated relativistic Breit-Wigner, i.e. quadratic in m.
4 : as 3, but the width is modified as for 2, and the current mass is used for its phase-space prefactor, i.e. m_0 Gamma_0 → m Gamma(m).

Note: this mode only applies to normal hadronic resonances like the rho. The more massive states of the isResonance() type, like Z^0 or top, are considered separately.

ParticleData:maxEnhanceBW   (default = 2.5; minimum = 1.; maximum = 5.)
The modifications in options 2 and 4 above enhance the large-mass tail of the Breit-Wigner distributions (the mass spectrum develops a dm/m divergence). However, we expect form factors to dampen this tail at masses some distance above the nominal one, so cut off the rise by requiring the actual Breit-Wigner weight not to be more than a factor maxEnhanceBW above the one obtained with options 1 or 3, respectively. This also opens up for a simpler technical handling of mass selection in options 2 and 4, by using standard hit-and-miss Monte Carlo.

Since running masses are only calculated for the six quark flavours, e.g. to obtain couplings to the Higgs boson(s), there is not an entry in the normal tables for each particles, but only the six MSbar mass values below, used as starting point for the running. In addition you can pick an alpha_s(M_Z), which is converted into a first-order five-flavour Lambda that is used to determine the rate of the running. (Without any match to four flavours below m_b; if desired, this can be fixed by slightly shifted default mass values, since the routines never should be called below the m_b scale anyway.)

ParticleData:mdRun   (default = 0.006; minimum = 0.003; maximum = 0.008)
the d quark MSbar mass at 2 GeV scale.

ParticleData:muRun   (default = 0.003; minimum = 0.001; maximum = 0.006)
the u quark MSbar mass at 2 GeV scale.

ParticleData:msRun   (default = 0.095; minimum = 0.060; maximum = 0.150)
the s quark MSbar mass at 2 GeV scale.

ParticleData:mcRun   (default = 1.25; minimum = 1.00; maximum = 1.50)
the c quark MSbar mass at the mass scale itself.

ParticleData:mbRun   (default = 4.20; minimum = 4.00; maximum = 4.50)
the b quark MSbar mass at the mass scale itself.

ParticleData:mtRun   (default = 165.0; minimum = 150.0; maximum = 175.0)
the t quark MSbar mass at the mass scale itself.

ParticleData:alphaSvalueMRun   (default = 0.125; minimum = 0.10; maximum = 0.20)
the alpha_s(M_Z) value used to define the rate at which MSbar masses run.

Comments on the data

Much of the current data has been updated based on the 2012 Review of Particle Physics [Ber12], while some is still based on the 2006 RPP [Yao06]. All known particle masses, widths and lifetimes have been set accordingly, while most not-yet-measured particles are kept at their values from PYTHIA 6. Decay channels and their branching ratios remain a major worry: many particles do not have one single solidly measured branching ratio, and many further do not have known branching ratios that add up to (the neighbourhood of) unity.

Uncertainties are especially big for the scalar, pseudovector and tensor L = 1 multiplets available in PYTHIA. We note that some distributions become better described when these multiplets are included in the generation, while others become worse. It is tempting to associate this lackluster performance with the primitive knowledge. Not even the multiplets themselves are particularly well known. It used to be that the a_0(980) and f_0(980) were considered to be members of the scalar multiplet. Nowadays they are commonly assumed to be either four-quark states or of some other exotic character. This means that the PYTHIA 8 PDG particle codes have been changed for these particles, relative to what was used in PYTHIA 6 based on previous PDG editions. Specifically their numbers are now in the 9000000 series, and they have been replaced in the scalar multiplet by a_0(1450) and f_0(1370).

For charm and bottom mesons the jungle of partial measurements makes it very difficult to construct fully consistent sets of decay channels. This part of the program has not yet been brought up to date to the 2006 RPP. Instead the LHCb decay tables (for EvtGen, but without using the EvtGen matrix-element machinery) and the DELPHI tune for PYTHIA 6 is being used. (This also includes a few non-c/b hadrons that only occur in the c/b decay tables.) This has the advantage that many tests have been made for consistency, but the disadvantage that it is not always in agreement with the latest measurements of some specific decay channels. The decays based on the LHCb tables (with some modifications) are 411, 421, 431, 441, 445, 511, 521, 531, 541, 3124, 4122, 4124, 5122, 10441, 10443, 13122, 14122, 20443, 23122, 30313, 30323, 30443, 33122, 100113, 100213, 100441, 100443, 100553, 9000111, 9000211. Correspondingly the decays based on the DELPHI tables are 415, 425, 435, 515, 525, 535, 4132, 4232, 4332, 5132, 5232 and 5332.

The data itself

Here comes the default particle data used in the program. Do not touch. The meaning of the various properties and the format used are explained ";?>here and the meMode codes ";?>here.

particle: id="0" name="void" spinType="0" chargeType="0" colType="0" m0="0.00000"

particle: id="1" name="d" antiName="dbar" spinType="2" chargeType="-1" colType="1" m0="0.33000"

particle: id="2" name="u" antiName="ubar" spinType="2" chargeType="2" colType="1" m0="0.33000"

particle: id="3" name="s" antiName="sbar" spinType="2" chargeType="-1" colType="1" m0="0.50000"

particle: id="4" name="c" antiName="cbar" spinType="2" chargeType="2" colType="1" m0="1.50000"

particle: id="5" name="b" antiName="bbar" spinType="2" chargeType="-1" colType="1" m0="4.80000"

particle: id="6" name="t" antiName="tbar" spinType="2" chargeType="2" colType="1" m0="171.00000" mWidth="1.40000" mMin="86.00000" mMax="0.00000"
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particle: id="22" name="gamma" spinType="3" chargeType="0" colType="0" m0="0.00000"

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